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Mathematical Analysis/Partial Differential Equations
Lifting default for S 1 -valued maps
Petru Mironescu
Université de Lyon, Université Lyon1, CNRS, UMR 5208, institut Camille-Jordan, bâtiment du Doyen Jean-Braconnier, 43, boulevard du 11 novembre 1918, 69200 Villeurbanne cedex, France
Received and accepted 30 July 2008 Available online 23 August 2008
Presented by Haïm Brezis
Abstract
Letϕ∈C∞([0,1]N,R). When 0< s <1,p1 and 1sp < N, theWs,p-semi-norm|ϕ|Ws,p ofϕis not controlled by
|g|Ws,p, whereg:=eıϕ[J. Bourgain, H. Brezis, P. Mironescu, Lifting in Sobolev spaces, J. Anal. Math. 80 (2000) 37–86]. [This question is related to existence, forS1-valued mapsg, of a liftingϕ as smooth as allowed byg.] In [J. Bourgain, H. Brezis, P. Mironescu, Lifting, degree, and distributional Jacobian revisited, Commun. Pure Appl. Math. 58 (2005) 529–551], the authors suggested that|g|Ws,pdoes control a weaker quantity, namely|ϕ|Ws,p+W1,sp. Existence of such control is due to J. Bourgain and H. Brezis [J. Bourgain, H. Brezis, On the equation divY =f and application to control of phases, J. Amer. Math. Soc. 16 (2003) 393–426] when 1< p2,s=1/pand to H.-M. Nguyen [H.-M. Nguyen, Inequalities related to liftings and applications, C. R.
Acad. Sci. Paris, Ser. I 346 (17–18) (2008) 957–962] whenN=1,p >1 andsp1 or whenN2,p >1 andsp >1. In this Note, we establish existence of control for alls <1,p1 andN.To cite this article: P. Mironescu, C. R. Acad. Sci. Paris, Ser. I 346 (2008).
©2008 Académie des sciences. Published by Elsevier Masson SAS. All rights reserved.
Résumé
Défaut de relèvement pour les applications à valeurs dans le cercle unité.Soitϕ∈C∞([0,1]N,R). Si 0< s <1,p1 et 1sp < N, alors la semi-norme|ϕ|Ws,p n’est pas contrôlée par|g|Ws,p, oùg:=eıϕ[J. Bourgain, H. Brezis, P. Mironescu, Lifting in Sobolev spaces, J. Anal. Math. 80 (2000) 37–86]. [Cette question est liée à l’existence, pour desgà valeurs dansS1, de relèvementsϕaussi réguliers quegle permet.] Dans [J. Bourgain, H. Brezis, P. Mironescu, Lifting, degree, and distributional Jacobian revisited, Commun. Pure Appl. Math. 58 (2005) 529–551], il est conjecturé que|g|Ws,pcontrôle une quantité plus faible que|ϕ|Ws,p, plus spécifiquement|ϕ|Ws,p+W1,sp. L’existence d’un tel contrôle est due à J. Bourgain and H. Brezis [J. Bourgain, H. Brezis, On the equation divY=f and application to control of phases, J. Amer. Math. Soc. 16 (2003) 393–426] pour 1< p2 ets=1/pet à H.-M. Nguyen [H.-M. Nguyen, Inequalities related to liftings and applications, C. R. Acad. Sci. Paris, Ser. I 346 (17–18) (2008) 957–962] pourN=1,p >1 etsp1 ou pourN2,p >1 etsp >1. Dans cette Note, nous montrons l’existence d’un contrôle pour touts <1,p1 etN.Pour citer cet article : P. Mironescu, C. R. Acad. Sci. Paris, Ser. I 346 (2008).
©2008 Académie des sciences. Published by Elsevier Masson SAS. All rights reserved.
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1631-073X/$ – see front matter ©2008 Académie des sciences. Published by Elsevier Masson SAS. All rights reserved.
doi:10.1016/j.crma.2008.08.001
Version française abrégée
SoientC= [0,1]N, 0< s <∞et 1p <∞.| |Ws,p désigne une semi-norme standard sur l’espace de Sobolev Ws,p(C); par exemple, pour 0< s <1 nous considérons la semi-norme de Gagliardo,
|u|Ws,p =
C2
|u(x)−u(y)|p
|x−y|N+sp dxdy 1/p
.
Si ϕ ∈C∞(C,R)etg:=eıϕ, alors |∇ϕ| = |∇g|. En particulier,|g|W1,p = |ϕ|W1,p. Plus généralement, |g|Ws,p
contrôle|ϕ|Ws,p sis1, au sens où il existe une inégalité de la forme|ϕ|Ws,p F (|g|Ws,p)avecF croissante [3].
Ceci n’est plus forcément vrai si 0< s <1. Voici un exemple inspiré de [3] : siN 2 et si 0< s <1 etp sont tels que 1< sp < N, alors il existe une fonction ψ∈W1,sp\Ws,p. Si on considère ϕε:=ψ∗ρε, avecρ noyau régularisant, alors|ϕε|Ws,p → ∞(carψ /∈Ws,p), alors quegε:=eıϕε reste bornée dansW1,sp∩L∞(carψ∈W1,sp) et donc dans Ws,p, grâce à l’inclusion de Gagliardo–NirenbergW1,sp∩L∞⊂Ws,p. Nonobstant la non inclusion W1,1∩L∞ ⊂Ws,psisp=1, on peut adapter cet exemple au cas oùsp=1 etN1. Plus généralement, sisp=1 ou 1< sp < N, alors on peut obtenir l’absence du contrôle à partir d’une fonction convenableψ∈Ws,p+W1,sp.
Dans le cas particuliers=1/2 etp=2, J. Bourgain et H. Brezis [2] ont montré que le contre-exemple ci-dessus est essentiellement le seul. Leur résultat est que toute fonctionϕ se décompose commeϕ=ϕ1+ϕ2, où|ϕ1|H1/2 et
|ϕ2|W1,1sont contrôlées par|g|H1/2. La preuve s’étend aux espacesW1/p,pavec 1< p2 et donne la décomposition (1). Ce résultat a motivé le problème suivant [4,8] avec 0< s <1 et 1p <∞:
(Ds,p) Toutϕ∈C∞(C,R)s’écritϕ=ϕ1+ϕ2, où|ϕ1|Ws,pC|eıϕ|Ws,p etDϕ2LspC|eıϕ|1/sWs,p.
Récemment, H.-M. Nguyen [10] a résolu ce problème lorsque p >1, s=1/petN =1 ; son argument s’applique aussi au casN2,p >1 etsp >1.
Le but de cette Note est d’annoncer le suivant :
Théorème 1.La décomposition(Ds,p)est valide pour tout0< s <1,p1etN.
Notons que la décomposition existe même sisp <1.
Idée de la preuve. On étendgà une applicationh:RN→R2, de sorte quehsoit Lipschitz, constante en dehors d’un compact,|h|3 et|h|Ws,p(RN)C|g|Ws,p(C). On étend ensuitehàRN×R∗+par la formulew(x, ε)=Π (h∗ρε(x)).
Ici,Π∈C∞(R2;R2)est telle queΠ (z)=z/|z|si|z|1/2, tandis queρ∈C0∞satisfaitρ0,
ρ=1, suppρ⊂ B(0,2)\B(0,1). Alors la conclusion du théorème est vérifiée parϕj données par
ϕ1(x):= − ∞
0
w(x, ε)∧∂w
∂ε(x, ε)dε, ϕ2:=ϕ−ϕ1.
L’inégalité|ϕ1|Ws,pC|h|Ws,p découle d’estimations standard1pour les régulariséesh∗ρεd’une fonctionh∈Ws,p. Elle implique|ϕ1|Ws,pC|g|Ws,p.
Pour estimerDϕ2, le point de départ est l’identité2
Dϕ2(x)= −2 ∞
0
∂
∂εw(x, ε)∧Dxw(x, ε)dε.
En adaptant une idée de [4], cette identité permet d’obtenir l’estimationDϕ2LspC|eıϕ|1/sWs,p. 2
1 L’une des estimations utilisées dans la preuve est RN∞
0 εp−sp−1|D[h∗ρε](x)|pdεdxC|h|pWs,p, bien connue par les spécialistes [11], II.12.
2 Évidente, du moins formellement.
Le lecteur trouvera les preuves détaillées dans [9] ; entre autres, on y explique pourquoi notre décomposition est une sorte d’analogue continu de la décomposition trouvée dans [2].
1. Introduction
LetC= [0,1]N, 0< s <∞and 1p <∞. We will denote by| |Ws,p a standard semi-norm on the Sobolev space Ws,p(C); e.g., when 0< s <1, we take the Gagliardo semi-norm
|u|Ws,p=
C2
|u(x)−u(y)|p
|x−y|N+sp dxdy 1/p
.
Letϕ∈C∞(C,R)and setg=eıϕ. Since|∇ϕ| = |∇g|, we have|g|W1,p= |ϕ|W1,p. More generally,|g|Ws,pcontrols
|ϕ|Ws,p when s1, i.e., there is some nondecreasing F such that |ϕ|Ws,p F (|g|Ws,p)[3]. This need not hold when 0< s <1. Here is an example, essentially taken from [3]: letN2 and let 0< s <1, 1p <∞be such that 1< sp < N. By a Sobolev “nonembedding”, there is someψ∈W1,sp\Ws,p. Letϕε:=ψ∗ρε and setgε= eıϕε, whereρ is a mollifier. Then|ϕε|Ws,p → ∞(since ψ /∈Ws,p). On the other hand, gε:=eıϕε is bounded in W1,sp∩L∞ (sinceψ∈W1,sp) and thus in Ws,p, by the Gagliardo–Nirenberg embeddingW1,sp∩L∞⊂Ws,p. Despite the nonembeddingW1,1∩L∞ ⊂Ws,pwhensp=1, one may easily adapt this example to the casesp=1 andN1. More generally, whensp=1 or 1< sp < N, one may prove lack of control with the help of an appropriate ψ∈Ws,p+W1,sp.
In the special cases=1/2 andp=2, J. Bourgain and H. Brezis [2] proved that the above counter-example is essentially the only one. Their results asserts that each ϕ splits as ϕ=ϕ1+ϕ2, where |ϕ1|H1/2 and|ϕ2|W1,1 are controlled by|g|H1/2. Their argument adapts steadily to the spacesW1/p,pwhere 1< p2 and yields
If 1< p2, thenϕ=ϕ1+ϕ2
whereϕj∈C∞(C), |ϕ1|W1/p,pC|g|W1/p,p, |ϕ2|W1,1C|g|pW1/p,p. (1) This motivated the following open problem [4,8]:
(Ds,p) Eachϕ∈C∞(C,R)splits asϕ=ϕ1+ϕ2, where|ϕ1|Ws,p C|eıϕ|Ws,p andDϕ2LspC|eıϕ|1/sWs,p. [Here, 0< s <1 and 1p <∞.] Very recently, H.-M. Nguyen [10] answered positively this problem whenp >1, s=1/pandN=1; his argument adapts to the case whereN2,p >1 andsp >1.
The main purpose of this Note is to announce the following:
Theorem 1.The decomposition(Ds,p)holds for each0< s <1,p1andN. Unlike the proofs in [2,10], our method applies to the casesp <1.
2. Heuristics of the proof of Theorem 1
In order to explain the main idea, we consider, for simplicity, maps defined onRN which are constant at infin- ity (rather than maps defined on [0,1]N). Assume first thatϕ has small amplitude oscillations, say|ϕ| 1. Then
|g−1| 1 and|ϕ|Ws,p ∼ |g|Ws,p. Thus, in this case, a convenient decomposition isϕ1=ϕ andϕ2=0. We next proceed as follows: we derive a formula forϕ. This formula givesϕ only whenϕ has small amplitude oscillations, but we may give it a meaning for eachϕ. In general (i.e., whenϕmay oscillate), we take this formula as the definition ofϕ1and simply letϕ2be the phase excess, i.e., we setϕ2=ϕ−ϕ1.
In order to obtain a tractable formula forϕ, we rely on the following remark: ifg=eıϕ, then there is no formula givingϕ in terms ofg, but there is one for Dϕ, since Dϕ=g∧Dg. We consider a smooth extension w:RN× [0,+∞[ →S1ofgsuch that
εlim→∞w(., ε)=const. (2)
A natural choice is w(x, ε)=Π (g∗ρε(x)), whereΠ (z)=z/|z| andρ is a mollifier. This yields a smooth map wheneverg(and thusg∗ρε) is close to 1. We may writew=eıψ, whereψ (x,0)=ϕ(x). Assuming that convergence in (2) is sufficiently fast, we than haveψ (x,∞)=Cand thus
ϕ(x)= −ψ (x, ε)|εε=∞=0 +C=C− ∞
0
w(x, ε)∧∂w
∂ε(x, ε)dε. (3)
As explained in the next section, (3) gives the right definition ofϕ1, provided we pick an appropriateρand we change slightly the definition ofΠ.
3. Sketch of the proof of Theorem 1
Let ϕ∈C∞(C,R)and set g=eıϕ. We first extend gto a Lipschitz map h:RN →R2 such thath is constant outside[−1,2]N,|h|3 and|h|Ws,p(RN)C|g|Ws,p(C). We next extendhtoRN×R∗+through the formulaw(x, ε)= Π (h∗ρε(x)). Here,Π∈C∞(R2;R2)is such thatΠ (z)=z/|z|if|z|1/2, whileρ∈C0∞satisfiesρ0,
ρ=1, suppρ⊂B(0,2)\B(0,1). Then the conclusion of the theorem holds withϕj given by
ϕ1(x):= − ∞
0
w(x, ε)∧∂w
∂ε(x, ε)dε, ϕ2:=ϕ−ϕ1. (4)
The inequality
|ϕ1|Ws,pC|h|Ws,p (5)
follows from standard estimates1for regularizationsh∗ρε of mapsh∈Ws,p. As a consequence of (5), we find that
|ϕ1|Ws,pC|g|Ws,p.
[Estimate (5) is a cousin of the estimate
x→ ∞
0
u∗ρε(x)∂
∂ε
v∗ρε(x) dε
Ws,p
CuL∞|v|Ws,p, (6)
valid for any reasonable ρ and presumably well known to experts. For specialρ’s, the “discrete” and much more popular analog of (6) is the “paraproduct inequality” [7]
jk
ujvk Ws,p
CuL∞|v|Ws,p, (7)
whereu=
uj,v=
jvj are the Littlewood–Paley decompositions ofuandv. Both (6) and (7) are refinements of the standard inequalityuvWs,pC(uWs,pvL∞+ vWs,puL∞).]
The starting point for estimatingDϕ2is the identity
Dϕ2(x)= −2 ∞
0
∂
∂εw(x, ε)∧Dxw(x, ε)dε. (8)
At least formally, this identity follows from
Dϕ2(x)=Dϕ(x)+ ∞
0
Dxw(x, ε)∧ ∂
∂εw(x, ε)dε+ ∞
0
w(x, ε)∧ ∂
∂εDxw(x, ε)dε
1 One of the key estimates used in the proof is RN∞
0 εp−sp−1|D[h∗ρε](x)|pdεdxC|h|pWs,p, well known to experts [11], II.12.
=w(x, ε)∧Dxw(x, ε)|ε=0+ ∞
0
Dxw(x, ε)∧ ∂
∂εw(x, ε)dε+w(x, ε)∧Dxw(x, ε)|εε=∞=0
− ∞
0
∂
∂εw(x, ε)∧Dxw(x, ε)dε= −2 ∞
0
∂
∂εw(x, ε)∧Dxw(x, ε)dε.
Adapting an idea from [4], this identity implies the estimateDϕ2LspC|eıϕ|1/sWs,p. 2 The interested reader will find the detailed proof in [9].
We end this section by comparing our decomposition to the Bourgain–Brezis one. Assuming, for the sake of the simplicity, thatϕandgare defined on the wholeRN, the decomposition in [2] is (withg=
gjthe Littlewood–Paley decomposition ofg)
ϕ1:=
jk
gj∧gk, ϕ2:=ϕ−ϕ1. (9)
In the same way (6) is related to (7), one may interpret the formula definingϕ1in (9) as a discrete analog of
x→ − ∞
0
g∗ρε(x)∧ ∂
∂ε
g∗ρε(x) dε.
Thus our decomposition is a continuous version of the one in [2], with the additional sophistication that the regular- izations ofgare “almost projected” ontoS1(viaΠ).
4. Some applications
As a first application, we may achieve the description ofXs,p=C∞(C;S1)Ws,p, partly obtained in [3] and [5].
Theorem 2.Let0< s <∞,1p <∞. Then
(a) ([3]) Whensp <1orspN,Xs,p=Ws,p(C;S1);
(b) ([5]) Whens1andsp2,Xs,p=Ws,p(C;S1);
(c) ([5]) Whens1and1sp <2,Xs,p= {eıϕ;ϕ∈Ws,p∩W1,sp(C,R)};
(d) When0< s <1and1< sp < N,Xs,p= {eıϕ;ϕ∈(Ws,p+W1,sp)(C,R)};
(e) When0< s <1,N2andsp=1,Xs,p= {eıϕ;ϕ∈(Ws,p+W1,1)(C,R)} ∩Ws,p(C;S1).
The lack of symmetry between statements (d) and (e) is explained by the fact that, whensp >1 ands <1, we have ϕ∈W1,sp⇒eıϕ∈Ws,p; this implication fails whensp=1 ands <1. For the proof of (d) and (e), we send the reader to [9].
In a forthcoming joint paper with H. Brezis and H.-M. Nguyen [6], we investigate several consequences of Theo- rem 1. We end this Note by mentioning one of them.
Theorem 3.(See [6].) Assume thatN3,0< s <1,2sp < N,k∈ {2,3, . . .}. Then, for eachu∈Ws,p(C;S1), there is somev∈Ws,p(C;S1)such thatu=vk.
This answers a question of F. Bethuel and D. Chiron [1]. [For the other values ofs,pandN, the surjectivity of the mapv→vkis clarified in [1]. The case considered in Theorem 3 is the only one left open in [1].]
Acknowledgements
The author thanks H.-M. Nguyen for sending him an early version of [10]. He warmly thanks P. Bousquet, H. Brezis and H.-M. Nguyen for useful discussions.
References
[1] F. Bethuel, D. Chiron, Some questions related to the lifting problem in Sobolev spaces, in: H. Berestycki, M. Bertsch, F. Browder, L. Nirenberg (Eds.), Perspectives in Nonlinear Partial Differential Equations, in: Contemporary Mathematics, vol. 446, Amer. Math. Soc., 2007, pp. 125–
152.
[2] J. Bourgain, H. Brezis, On the equation divY=f and application to control of phases, J. Amer. Math. Soc. 16 (2003) 393–426.
[3] J. Bourgain, H. Brezis, P. Mironescu, Lifting in Sobolev spaces, J. Anal. Math. 80 (2000) 37–86.
[4] J. Bourgain, H. Brezis, P. Mironescu, Lifting, degree, and distributional Jacobian revisited, Commun. Pure Appl. Math. 58 (2005) 529–551.
[5] H. Brezis, P. Mironescu, On some questions of topology forS1-valued fractional Sobolev spaces, Rev. R. Acad. Cien., Serie A Mat. 95 (2001) 121–143.
[6] H. Brezis, P. Mironescu, H.-M. Nguyen, in preparation.
[7] J.-Y. Chemin, Fluides parfaits incompressibles, Astérisque 230 (1995).
[8] P. Mironescu, Sobolev maps on manifolds: degree, approximation, lifting, in: H. Berestycki, M. Bertsch, F. Browder, L. Nirenberg, L.A.
Peletier, L. Véron (Eds.), Perspectives in Nonlinear Partial Differential Equations, In honor of Haïm Brezis, in: Contemporary Mathematics, vol. 446, Amer. Math. Society, 2007, pp. 413–436.
[9] P. Mironescu, Lifting ofS1-valued maps in sums of Sobolev spaces, J. European Math. Soc., submitted for publication.
[10] H.-M. Nguyen, Inequalities related to liftings and applications, C. R. Acad. Sci. Paris, Ser. I 346 (17–18) (2008) 957–962.
[11] H. Triebel, Theory of Function Spaces, Birkhäuser Verlag, 1983.